New Angular-Shaped and Isomerically Pure Anthradithiophene with

May 23, 2012 - Department of Applied Chemistry, National Chiao Tung University, 1001 Ta ..... layer in BHJ-PSC with a multi-functional solid organic a...
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New Angular-Shaped and Isomerically Pure Anthradithiophene with Lateral Aliphatic Side Chains for Conjugated Polymers: Synthesis, Characterization, and Implications for Solution-Prossessed Organic Field-Effect Transistors and Photovoltaics Jhong-Sian Wu, Chung-Te Lin, Chien-Lung Wang, Yen-Ju Cheng,* and Chain-Shu Hsu* Department of Applied Chemistry, National Chiao Tung University, 1001 Ta Hsueh Road, Hsin-Chu, 30010 Taiwan S Supporting Information *

ABSTRACT: An isomerically pure anti-anthradithiophene (aADT) arranged in an angular shape is developed. Formation of the framework of aADT incorporating four lateral alkyl substituents was accomplished by a one-pot benzannulation via multiple Suzuki coupling. This newly designed 2,8-stannylated aADT monomer was copolymerized with a ditheniodiketopyrrolopyrrole (DPP) unit and a bithiophene unit, respectively, to furnish an alternating donor−acceptor copolymer poly(anthradithiophene-alt-dithienyldiketopyrrolopyrrole) (PaADTDPP) and a thiophene-rich poly(anthradithiophene-alt-bithiophene) (PaADTT). PaADTT with crystalline nature achieved a high FET mobility of 7.9 × 10−2 cm2 V−1 s−1 with an on−off ratio of 1.1 × 107. The photovoltaic device based on the PaADTDPP:PC71BM (1:2.5, w/w) blend exhibited a Voc of 0.66 V, a Jsc of 9.49 mA/cm2, and a FF of 58.4%, delivering a power conversion efficiency (PCE) of 3.66%. By adding 1.5 vol % 1-chloronaphthalene (CN) as a processing additive, the PCE can be improved to 4.24%. We demonstrated that these angular-shaped and alkylated aADT-based polymers have better organic photovoltaic (OPVs) and fieldeffect transistor (FETs) characteristics than the linear-shaped ADT-containing polymers. KEYWORDS: anthradithiophene, benzannulation, solar cells, field-effect transistors

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INTRODUCTION Solution-processed organic photovoltaics (OPVs) and organic field-effect transistors (OFETs) have received tremendous scientific and industrial interest in recent years due to their cost-effective and mechanically flexible advantages.1 Development of advanced p-type conjugated polymers continues to play a pivotal role to drive high efficiency of OPVs and high mobility of OFETs. Considerable effort has been devoted to designing and synthesizing multifused aromatic small molecules, which can ultimately be used to construct solutionprocessable conjugated polymers.2 The acenedithiophene family, where polyaromatic benzene rings are fused with two terminal thiophene rings, are particularly attractive and promising building blocks.3 First, α-positions of the two endcapped thiophenes can be selectively functionalized for easy and precise cross-coupling polymerization. Second, integration of thiophene and benzene rings into a rigid and coplanar entity facilitates π-electron delocalization and induces strong π−π stacking for efficient charge transporting.4 Third, the aromatic size and molecular shape of the acenedithiophene system are chemically manipulable to tailor the electronic and steric properties.3a,4a,c Incorporation of the shortest acenedithiophenes, that is, benzodithiophene (BDT), into a variety of conjugated polymers has produced highly efficient organic fieldeffect transistors (OFETs) and bulk heterojunction (BHJ) polymer solar cells (PSCs).3b,5 Pentacene is the most © 2012 American Chemical Society

representative semiconductor to realize the highest mobility of OFETs but is also known for being poorly stable against photoinduced oxidation.6 Linear-fused anthradithiophene (lADT) derivatives not only exhibit comparable OFET mobilities to pentacene but also possess many advantages, including easier functionalization, broader absorption window, and better chemical stability.4d,e,7 Nevertheless, the polymers incorporating lADT units are only sporadically reported.8 One problem at the molecular level is that introducing two alkyl chains on the 5, 10 positions of lADT units is not sufficient to warrant solubility of the resulting polymers for solutionprocessing. Furthermore, the traditional synthesis of the linearfused ADT inevitably afforded an inseparable mixture of syn- and anti-isomers resulting in undefined molecular conformation.7c,9 So far the PSC devices using the lADT-based polymers have only shown power conversion efficiencies (PCE) less than 1%.8 Recently, Takimiya and co-workers demonstrated that the shape of the naphthodithiophene (NDT) motif plays a critical role in polymer packing (Scheme 1).10 In contrast to the polymer with the linear-fused NDT units, the copolymer incorporating the angular-fused NDT units can pack into highly ordered structures, thereby achieving higher FET mobilities. Received: April 17, 2012 Revised: May 18, 2012 Published: May 23, 2012 2391

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Scheme 1. Chemical Structures of Acenedithiophene Derivatives, BDT, lNDT, aNDT, lADT, aADT, and Laterally Alkylated aADT

Scheme 2. Chemical Structures of the Anthradithiophene-Based Copolymers, PaADTDPP and PaADTT

by Negishi coupling of (3-bromothiophen-2-yl)zinc(II)bromide (5) with 1,4-dibromo-2,5-diiodobenzene (6).13 In the presence of Pd(PPh3)4 as the catalyst, aADT was successfully synthesized by tandem Suzuki-Miyaura cross-coupling of 7 with diborylalkene (3) in good reaction yield of 59%.14 This strategy is very efficient and useful in view of forming the aADT framework with concomitantly introducing four flanking octyl chains. It is also the first example that double benzannulation by Suzuki coupling can be carried out through a benzenethiophene-type dibromobiaryl substrate. Note that the length of alkyl chains can be easily adjustable depending on preparation of the dialkyldiborylalkene analogues. Lithiation of aADT by t-butyllithium to react with trimethyltin chloride resulted in the formation of Sn-aADT in almost quantitative yield (99%). Monomer Sn-aADT was copolymerized with 3,6-bis(5bromothiophen-2-yl)-2,5-bis(2-ethylhexyl)pyrrolo[3,4-c]pyrrole-1,4(2H,5H)-dione (8) and 5,5′-dibromo-4,4′-ditetradecyl-2,2′-bithiophene (9) by Stille coupling to give PaADTDPP and PaADTT, respectively (Scheme 3). The molecular weights of PaADTDPP and PaADTT are not obtainable due to their low solubilities in tetrahydrofuran at room temperature. Thermal Properties. The thermal stability was analyzed by thermogravimetric analysis (TGA). PaADTDPP and PaADTT exhibited sufficiently high decomposition temperatures (Td) of 400 and 434 °C, respectively, indicating that PaADTT is thermally more stable than PaADTDPP (Figure S1 in Supporting Information). On the basis of the differential scanning calorimetry (DSC) analysis, PaADTDPP is amorphous, while bithiophene-based PaADTT showed crystalline nature with the observation of the melting point at 285 °C during heating and the crystallization point at 276 °C upon cooling (Figure 1).

It was also reported that angular-fused ADT (aADT) has a lowerlying HOMO energy level than lADT, which could be beneficial for better air stability and greater open-circuit voltage (Voc) for PSCs.3a On the basis of the aforementioned considerations, it is promising and desirable to develop an angular-fused ADT for preparing a new class of ADT-based polymers for FET as well as OPV applications (Scheme 1). Despite the fact that the synthesis of the angular-shaped aADT small molecule has been reported previously,11 the absence of aliphatic side chains as solubilizing groups restricted its practical application for polymer synthesis. To circumvent this deficiency, we present here a useful and facile synthesis to prepare an isomer-free aADT with the implantation of four lateral alkyl substituents at its 4, 5 and 10, 11 positions (Scheme 1). The synthesis of aADT is simply accomplished by one-pot benzannulation via multiple Suzuki coupling. This newly designed 2,8-stannylated aADT monomer was copolymerized with a dithienodiketopyrrolopyrrole (DPP) unit and a bithiophene unit, respectively, to furnish an alternating donor−acceptor copolymer poly(anthradithiophene-alt-dithienyldiketopyrrolopyrrole) (PaADTDPP) and a thiophene-rich poly(anthradithiophene-alt-bithiophene) (PaADTT) (Scheme 2). The synthesis, characterization, and applications of these polymers in PSCs and FETs will be discussed.

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RESULTS AND DISCUSSION Synthesis of Monomers and Polymers. The synthesis of the monomers Sn-aADT is depicted in the Scheme 3. Lithiation of 1-decyne (1) was followed by reacting with 1-bromooctane yielded 9-octadecyne (2). Pt-catalyzed syn-diborylation of bis(pinacolato)diboron with 2 afforded dioctyl-bis(pinacolatoboryl)alkene (3) in 75% yield.12 The 2,2′-(2,5dibromo-1,4-phenylene)bis(3-bromothiophene) (7) was prepared 2392

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Scheme 3. Synthetic Route for the Angular-Fused Anthradithiophene Unit and the Corresponding Copolymers

Figure 1. Differential scanning calorimetry of PaADTDPP (a) and PaADTT (b).

Optical Absorption. The absorption spectra of the monomer and polymers are shown in Figure 2. The absorption spectrum of the aADT monomer consists of three sharp peaks with narrow bandwidth (Figure 2a). Besides, small bands at lower energy of 362, 383, and 403 nm, which are presumably attributed to vibronic transitions, in toluene solution were also observed. These characteristics clearly reflect the highly rigid and coplanar feature of the anthradithiophene unit. For PaADTDPP, the shorter wavelength absorbance comes from the π−π* transition of the pentacyclic units, while the lower energy band is ascribed to the intramolecular charge transfer (ICT) between the electron-rich and the electron-deficient

DPP unit (Figure 2b). The donor−acceptor PaADTDPP copolymer showed a narrow optical band gap (1.39 eV) deduced from the absorption edge of solid state spectra. Besides, PaADTDPP showed a tailing of the absorption band with a shoulder around 850 nm in the solid state. The origin of this shoulder presumably comes from strong intermolecular interactions. The absorption spectra of PaADTDPP in the solution and solid states are essentially unchanged, whereas PaADTT showed significant red-shifted absorption in the solid state due to the stronger π−π stacking and higher degree of the intermolecular ordering (Figure 2c). Also note that a new shoulder peak at 553 nm is developed in the solid state. These 2393

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phenomena are rather consistent with the crystalline nature of PaADTT. Electrochemical Properties. Cyclic voltammetry (CV) was employed to examine the electrochemical properties and evaluate the highest occupied molecular orbital (HOMO) and lowest unoccupied molecular orbital (LUMO) levels of the polymers (Table 1 and Figure 3). The two polymers showed

Figure 3. Cyclic voltammograms of PaADTDPP and PaADTT in the thin film at a scan rate of 50 mV/s.

stable and reversible p-doping/n-doping process in the cathodic and anodic scans. The HOMO levels being estimated to be −5.21 eV for PaADTDPP and −5.41 eV for PaADTT are at ideal range to ensure better air stability and greater attainable Voc in the final device. The LUMO level is located at −3.61 eV for PaADTDPP, which is positioned 0.2 eV above the LUMO level of the PC71BM (−3.8 eV) to induce energetically favorable electron transfer. However, the LUMO energy level of PaADTT is −3.0 eV, which might be too high relative to the LUMO level of PC71BM. Characteristics of Organic Field-Effect Transistors. To evaluate the FET hole mobilities of the aADT-based polymers, the devices using a bottom-gate, top-contact configuration with evaporated gold source/drain electrodes (40 nm in thickness) were fabricated. The output and transfer plots of the devices exhibited typical p-channel OFET characteristics (Figure 4). The hole mobilities were deduced from the transfer characteristics of the devices in the saturation regime. The PaADTDPPbased OFETs using unmodified SiO2 as gate dielectric produced the hole motilities of 2.0 × 10−3 and 9.4 × 10−3 cm2 V−1 s−1 with the annealing temperature at 150 and 250 °C, respectively (Table 2). To further improve the device characteristics, the surface of the SiO2 gate dielectric was treated with octadecyltrichlorosilane (ODTS) to form a selfassembled monolayer (SAM). With the modification of a ODTS-SAM layer, the hole mobilities of the PaADTDPP

Figure 2. Normalized absorption spectra of aADT in toluene solution (a), PaADTDPP (b), and PaADTT (c) in o-dichlorobenzene (ODCB) solution and the solid state.

Table 1. Summary of the Intrinsic Properties of the Polymers λmax (nm)

a

polymer

Td (°C)

Tm (°C)

Egopta (eV) (Film)

ODCB

film

HOMO (eV)

LUMO (eV)

Egecb

PaADTDPP PaADTT

400 434

285

1.39 2.13

368, 736 318, 390, 479

368, 670, 736 314, 406, 513, 553

−5.21 −5.41

−3.61 −3.00

1.60 2.41

Egopt from the onset of UV spectra in thin film. bEgec = electrochemical band gap (LUMO−HOMO). 2394

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Figure 4. Typical output curves (a, c) and transfer plots (b, d) of the OFET devices based on PaADTDPP and PaADTT with ODTS-SAM layer, respectively.

Table 2. p-Type FET Characteristics of PaADTDPP and PaADTT Film polymer

SAM layer

annealing (°C)

PaADTDPP PaADTDPP PaADTDPP PaADTDPP PaADTT PaADTT PaADTT PaADTT

bare SiO2 bare SiO2 ODTS ODTS bare SiO2 bare SiO2 ODTS ODTS

150 250 150 250 150 250 150 250

mobility (cm2 V−1 s−1) 2.0 9.4 2.2 7.3 7.2 1.2 7.9 6.8

devices were significantly enhanced to 2.2 × 10−2 cm2 V−1 s−1 and 7.3 × 10−2 cm2 V−1 s−1 with the annealing temperature at 150 and 250 °C, respectively. Accordingly, the on−off ratios were also dramatically improved to 5.2 × 105 and 1.6 × 106. On the other hand, the mobilities of the PaADTT-based devices did not show distinct correlation with respect to the annealing temperatures. It was found that the PaADTT hole mobility is only slightly higher in the ODTS-modified device than the unmodified one due to the reason that order π−π stacking can also be formed on the bare SiO2 due to the crystalline nature of PaADTT. PaADTT achieved the highest mobility of 7.9 × 10−2 cm2 V−1 s−1 with an on−off ratio of 1.1 × 107 from the ODTS-modified device annealed at 150 °C. Photovoltaic Characteristics. Bulk heterojunction PSCs were fabricated on the basis of ITO/PEDOT:PSS/polymer:PC71BM/Ca/Al configuration, and their performances were measured under 100 mW/cm2 AM 1.5 illumination. The characterization data are summarized in Table 3, and the current density−voltage characteristics of these polymers are shown in Figure 5. The device based on the

× × × × × × × ×

10−3 10−3 10−2 10−2 10−2 10−2 10−2 10−2

I (on/off)

Vt (V)

× × × × × × × ×

18.8 25.2 −2.9 −8.2 −6.0 −4.4 −13.0 −7.3

3.1 1.8 5.2 1.6 5.1 1.9 1.1 1.5

103 102 105 106 106 106 107 108

Table 3. PSCs Characteristics of PaADTDPP and PaADTT

a

polymer

blend ratio with PC71BM

Voc (V)

Jsc (mA/cm2)

FF (%)

PCE (%)

PaADTDPP PaADTDPP PaADTT

1:2.5 1:2.5a 1:1

0.66 0.66 0.80

9.49 10.66 3.46

58.4 60.2 63.8

3.66 4.24 1.77

1-Chloronaphthalene (1.5 vol %) in ODCB solution.

PaADTDPP:PC71BM (1:2.5, w/w) blend exhibited a Voc of 0.66 V, a Jsc of 9.49 mA/cm2, and a FF of 58.4%, delivering an PCE of 3.66%. By judicial choice of the processing additives, nanoscale morphology of the active layer can be efficiently controlled and optimized.2b,15 Encouragingly, by adding 1.5 vol % 1-chloronaphthalene (CN) into ODCB as the processing additive, the PCE was improved to 4.24% as a result of the increased Jsc values. To gain more insight into the performance enhancement upon the introduction of CN additive, the morphology of the blend films was investigated by atomic force microscope (AFM) (Figure 6). Compared to the pristine film, 2395

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higher Voc of 0.80 V due to the lower-lying HOMO level (−5.41 eV). However, the much lower Jsc resulting in the lower PCE might be due to the limited absorption range of PaADTT or energetically unfavorable charge transfer.

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CONCLUSIONS

Structurally analogous to pentacene, linear-fused anthradithiophene derivatives have received a great deal of interest due to their high intrinsic mobilities and good chemical stability. However, compared to the devices based on lADT small molecules, solution-processable lADT-based conjugated polymers have not produced successful OPV and OFET device performance. Introducing sufficient aliphatic side chains to improve solubility and modulating molecular shape of the ADT system to optimize molecular packing provide effective solutions to overcome the deficiencies. In this regard, we have developed an elegant route to synthesize an angularshaped and isomer-free anti-anthradithiophene moiety. The merit of the synthesis is that the construction of aADT framework and the introduction of aliphatic side chains are accomplished simultaneously by one-pot Suzuki-coupling benzannulation between a dialkyldiborylalkene and a dibromobiaryl substrate. For the first time, the aADT unit was copolymerized with DPP and bithiophene monomers to prepare aADT-based conjugated polymers, PaADTDPP and PaADTT, respectively. The OPV device based on PaADTDPP/PC71BM delivered a decent PCE of 4.24%, which is the highest value among the devices using the lADT-based polymers. Besides, PaADTT also achieved a high

Figure 5. Current density−voltage characteristics of ITO/PEDOT:PSS/polymer:PC71BM/Ca/Al devices under illumination of AM 1.5 G at 100 mW/cm2.

the additive-processed PaADTDPP:PC71BM film showed small phase separation domains and more pronounced fiber-like nanostructures with greater surface roughness, suggesting its more favorable morphological property for efficient charge separation and transporting properties. On the other hand, the device using the PaADTT/PC71BM blend (1:1, w/w) exhibited a Voc of 0.80 V, a Jsc of 3.46 mA/cm2, and a FF of 63.8%, leading to a PCE of 1.77%. Compared to PaADTDPP, the device based on PaADTT as the p-type material exhibited a

Figure 6. AFM height and phase images of the surface of PaADTDPP/PC71BM blend (a, b) and PaADTDPP/PC71BM (with 1.5 vol % CN) (c, d). 2396

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FET mobility of 7.9 × 10−2 cm2 V−1 s−1 with an on−off ratio of 1.1 × 107, which also outperforms the lADT-containing polymers reported in the literature.8b Further optimization of the molecular properties of aADT-based polymers is highly achievable by modification of aliphatic substituents on aADT, or by copolymerization of the aADT monomer with various acceptors. Finally, this synthetic strategy will also be applicable for creating a range of new fascinating ladder-type conjugated structures. The follow-up research is currently underway in our laboratory.

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characteristics of PSC devices were obtained by a Keithley 2400 SMU. Solar illumination conforming the JIS Class AAA was provided by a SAN-EI 300W solar simulator equipped with an AM 1.5G filter. The light intensity was calibrated with a Hamamatsu S1336-5BK silicon photodiode. Synthesis of 9-Octadecyne (2). To a solution of 1-decyne 1 (6.0 g, 43.4 mmol) in dry THF (60 mL) was added a 2.0 M solution of lithium diisopropylamide (LDA) in hexane (23.9 mL, 47.8 mmol) dropwise at 0 °C. After stirring at 0 °C for 1 h, 1-bromooctane (8.8 g, 45.6 mmol) was introduced by syringe to the solution. The mixture solution was warmed up to room temperature and refluxed at 60 °C for 12 h. The mixture solution was quenched with water and extracted with diethyl ether (100 mL × 3) and water (100 mL). The combined organic layer was dried over MgSO4. After removal of the solvent under reduced pressure, the residue was distilled at 150 °C to remove impurities. The residue was purified by column chromatography on silica gel (hexane) to give a colorless liquid 2 (2.7 g, 25%). 1H NMR (CDCl3, 300 MHz, ppm): δ 0.88 (t, J = 6.6 Hz, 6 H), 1.27−1.38 (m, 20 H), 1.45−1.49 (m, 4 H), 2.13 (t, J = 6.9 Hz, 4 H). 13C NMR (CDCl3, 75 MHz, ppm): δ 14.23, 18.91, 22.82, 29.04, 29.31, 29.34, 29.40, 32.02, 80.35. MS (EI, C18H34): calcd, 250.46; found, 250. Synthesis of (Z)-1,2-Bis(4,4,5,5-tetramethyl-1,3,2-dioxaborolan-2-yl)-1,2-dioctylethene (3). The compound was synthesized by following the procedure in the literature.12 9-Octadecyne 2 (2.5 g, 9.98 mmol), bis(pinacolato)diboron (2.3 g, 9.07 mmol) and Pt(PPh3)4 (339 mg, 0.27 mmol) were dissolved in DMF (40 mL). The reaction mixture was stirred at 80 °C for 24 h and then extracted with diethyl ether (100 mL × 3) and water (150 mL). The collected organic layer was dried over MgSO4. After removal of the solvent under reduced pressure, the residue was purified by column chromatography on silica gel (hexane/ethyl acetate, v/v, 25/1) to give a colorless liquid 3 (3.77 g, 75%). 1H NMR (CDCl3, 300 MHz, ppm): δ 0.85−0.89 (m, 6 H), 1.21−1.31 (m, 48 H), 2.16 (t, J = 7.5 Hz, 4 H). 13C NMR (CDCl3, 75 MHz, ppm): δ 14.24, 22.83, 25.03, 29.36, 29.62, 29.88, 30.16, 30.97, 32.05, 83.36. MS (EI, C30H58B2O4): calcd, 504.4; found, 504. Elemental analysis (%) calcd for C30H58B2O4: C, 71.44; H, 11.59. Found: C, 71.23; H, 11.34. Synthesis of (3-Bromothiophen-2-yl)zinc(II)bromide (5). To a solution of 2,3-dibromothiophene 4 (6.25 g, 25.8 mmol) in dry THF (20 mL) was added a 2.5 M solution of n-BuLi in hexane (11.1 mL, 27.7 mmol) dropwise at −78 °C. After stirring at −78 °C for 1 h, the mixture solution was warmed up to room temperature. The mixture solution was added to a solution of zinc(II)bromide (5.82 g, 25.8 mmol) in dry THF (15 mL) at −78 °C, and then the mixture solution was stirred at 0 °C for 1 h. Synthesis of 2,2′-(2,5-Dibromo-1,4-phenylene)bis(3-bromothiophene) (7). To a solution of 1,4-dibromo-2,5-diiodobenzene 6 (4.50 g, 9.2 mmol) and Pd(PPh3)4 (0.27 g, 0.23 mmol) in dry THF (30 mL) was added a solution of (3-bromothiophen-2-yl)zinc(II)bromide 5 (25.8 mmol) at room temperature. The mixture solution was refluxed for 3 h. After removal of the solvent under reduced pressure, the residue was extracted with ethyl acetate (250 mL × 3) and water (150 mL). The collected organic layer was dried over MgSO4. After removal of the solvent under reduced pressure, the residue was purified by column chromatography on silica gel (hexane) to give a white solid product 7 (1.54 g, 30%). 1H NMR (CDCl3, 300 MHz, ppm): δ 7.09 (d, J = 5.4 Hz, 2 H), 7.42 (d, J = 5.4 Hz, 2 H), 7.71 (s, 2 H). 13C NMR (CDCl3, 75 MHz, ppm): δ 111.79, 123.53, 126.97, 130.51, 135.19, 136.13, 136.64. Synthesis of aADT. The compound was synthesized by following the procedure in the literature.14 2,2′-(2,5-Dibromo-1,4-phenylene)bis(3-bromothiophene) 7 (500 mg, 0.90 mmol), (Z)-1,2-bis(4,4,5,5tetramethyl-1,3,2-dioxaborolan-2-yl)-1,2-dioctylethene 3 (1.04 g, 2.06 mmol), K2CO3 (1.49 g, 10.78 mmol), and Pd(PPh3)4 (104 mg, 0.09 mmol) were dissolved in deoxygenated THF/H2O (40 mL/2.1 mL). The mixture was then degassed by bubbling nitrogen for 5 min at room temperature. The reaction mixture was refluxed at 65 °C for 48 h and then extracted with diethyl ether (100 mL × 3) and water (150 mL). The collected organic layer was dried over MgSO4. After removal of the solvent under reduced pressure, the residue was

EXPERIMENTAL SECTION

General Measurement and Characterization. All chemicals are purchased from Aldrich or Acros and used as received unless otherwise specified. 1H and 13C NMR spectra were measured using a Varian 300 MHz instrument spectrometer. Differential scanning calorimeter (DSC) was measured on a TA Q200 Instrument, and thermogravimetric analysis (TGA) was recorded on a Perkin-Elmer Pyris under nitrogen atmosphere at a heating rate of 10 °C/min. Absorption spectra were collected on a HP8453 UV−vis spectrophotometer. The molecular weights of the polymers were measured by the GPC method on a Viscotek VE2001GPC, and polystyrene was used as the standard (THF as the eluent). The electrochemical cyclic voltammetry (CV) was conducted on a CH Instruments Model 611D. A carbon glass coated with a thin polymer film was used as the working electrode and Ag/Ag+ electrode as the reference electrode, while 0.1 M tetrabutylammonium hexafluorophosphate (Bu4NPF6) in acetonitrile was the electrolyte. CV curves were calibrated using ferrocence as the standard, whose oxidation potential is set at −4.8 eV with respect to the zero vacuum level. The HOMO energy levels were obtained from the equation HOMO = −(Eoxonset − E(ferrocene)onset + 4.8) eV. The LUMO levels of polymer were obtained from the equation LUMO = −(Eredonset − E(ferrocene)onset + 4.8) eV. OFET Fabrication. An n-type heavily doped Si wafer with a SiO2 layer of 300 nm and a capacitance of 11 nF/cm2 was used as the gate electrode and dielectric layer. Thin films (40−60 nm in thickness) of polymers were deposited on octadecyltrichlorosilane (ODTS)-treated SiO2/Si substrates by spin-coating their o-dichlorobenzene solutions (5 mg/mL). Then, the thin films were annealed at different temperatures (150 or 250 °C) for 30 min. Gold source and drain contacts (40 nm in thickness) were deposited by vacuum evaporation on the organic layer through a shadow mask, affording a bottom-gate, top-contact device configuration. Electrical measurements of OTFT devices were carried out at room temperature in air using a 4156C, Agilent Technologies. The field-effect mobility was calculated in the saturation regime by using the equation Ids = (μWCi/2L)(Vg − Vt)2, where Ids is the drain-source current, μ is the field-effect mobility, W is the channel width (1 mm), L is the channel length (100 μm), Ci is the capacitance per unit area of the gate dielectric layer, Vg is the gate voltage, and Vt is threshold voltage. PSCs Fabrication. ITO/glass substrates were ultrasonically cleaned sequentially in detergent, water, acetone, and iso-propanol (IPA). The cleaned substrates were covered by a 30 nm thick layer of PEDOT:PSS (Clevios P provided by Stark) by spin coating. After annealing in a glovebox at 150 °C for 30 min, the samples were cooled to room temperature. Polymers were dissolved in o-dichlorobenzene (ODCB) or 1.5 vol % 1-chloronaphthalene (CN) ODCB solution, and then PC71BM (purchased from Nano-C) was added. The solution was then heated at 80 °C and stirred overnight at the same temperature. Prior to deposition, the solution were filtered (1 μm filters). The solution of polymer:PC71BM was then spin coated to form the active layer. The cathode made of calcium (350 nm thick) and aluminum (1000 nm thick) was sequentially evaporated through a shadow mask under high vacuum (